Integrating Exponential Functions to Solving e^(-(x^2)/2)

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Discussion Overview

The discussion revolves around the integration of the function e^(-(x^2)/2), exploring various methods and approaches to solve the integral, including power series expansion and substitution techniques. Participants also discuss related integrals, such as the Gaussian integral and the error function, within the context of both definite and indefinite integrals.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest using the power series expansion of e^x to approach the integration of e^(-(x^2)/2), while others argue that this method does not yield a closed form solution.
  • One participant proposes substituting u = (-(x^2)/2) to transform the integral into a more manageable form, but others challenge the feasibility of this substitution due to the presence of x^2.
  • It is noted that the integral from negative infinity to positive infinity of e^(-x^2) equals √π, with a proof involving polar coordinates presented by a participant.
  • Another participant claims that the integral of e^(-x^2/2) from negative infinity to positive infinity equals √(2π), while a different participant suggests it equals √(π/2), leading to disagreement.
  • Concerns are raised about the divergence of the integral of e^(x^2) and whether it can be evaluated over finite intervals, with some suggesting that it would diverge if taken from negative infinity to positive infinity.
  • Participants discuss the use of the error function in relation to the Gaussian integral, with some expressing uncertainty about the validity of certain substitutions in their calculations.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the integration of e^(-(x^2)/2) and related integrals. There is no consensus on the correct evaluation of the integral from negative infinity to positive infinity, as differing results are presented.

Contextual Notes

Limitations include unresolved mathematical steps, particularly regarding the validity of substitutions and the conditions under which certain integrals converge or diverge. The discussion also highlights the dependence on definitions of integrals and the error function.

d_b
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Hi!

I want to know how to intergrat e^(-(x^2)/2) . Someone told me to use the intergration of e^x= 1+ x + (x^2) /2!+ ...(X^n)/n! ... is that sounds right?? and if it is i got pi as an answer for e^(-(x^2)/2) , is that the right answer?
 
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We know that \int{e^x}dx = e^x so try to get it into that form. Substitute u = (-(x^2)/2) and get \int{e^u}du = e^u * du/dx. Solving du/dx gives you -x. You should get an answer of -xe^((-x^2)/2) - I'm pretty sure, anyway.
 
d_b said:
Hi!

I want to know how to intergrat e^(-(x^2)/2) . Someone told me to use the intergration of e^x= 1+ x + (x^2) /2!+ ...(X^n)/n! ... is that sounds right?? and if it is i got pi as an answer for e^(-(x^2)/2) , is that the right answer?

e-x2 cannot be integrated (indefinite) analytically. If you expand it into a power series, you can get the power series of the integral. There is no closed form solution.
The integral (-oo,x) (divided by sqrt(2pi)) is called erf(x).
 
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dprimedx said:
We know that \int{e^x}dx = e^x so try to get it into that form. Substitute u = (-(x^2)/2) and get \int{e^u}du = e^u * du/dx. Solving du/dx gives you -x. You should get an answer of -xe^((-x^2)/2) - I'm pretty sure, anyway.

I don't think you can intergrate it like that because you have x^2 and so when trying to use another variable du it will gives dx equals du*fraction of x and you can't solve for x then
 
mathman said:
e-x2 cannot be integrated (indefinite) analytically. If you expand it into a power series, you can get the power series of the integral. There is no closed form solution.
The integral (-oo,x) (divided by sqrt(2pi)) is called erf(x).

I actually meant to intergrate from negative infinity to positive infinity.
 
The answer is

\int_{-\infty}^{\infty} e^{-x^2} \,dx = \sqrt{\pi}.Here's a proof: Let

I = \int_{-\infty}^{\infty} e^{-x^2} \,dx = \sqrt{\pi}.

Clearly I is positive, so if we can show that I^2 = \pi[/tex] we are done:<br /> <br /> I^2 = \left(\int_{-\infty}^{\infty} e^{-x^2} \,dx \right) \left(\int_{-\infty}^{\infty} e^{-y^2} \,dy \right)&lt;br /&gt; = \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-(x^2 + y^2)} \,dx \,dy.<br /> <br /> Switching to polar coordinates (r, \theta), we have x^2 + y^2 = r^2 and dx\,dy = r\,dr\,d\theta. Thus,<br /> <br /> I^2 = \int_{0}^{2\pi} \int_{0}^{\infty} r e^{-r^2} \,dr \,d\theta.<br /> <br /> Substituting u = -r^2 so that r \,dr = -du/2 will give the result.
 
Thank you for clearing up the problem, I haven't learn how to do double intergral yet so is there any other way of doing it without using double intergral??

also \int_{-\infty}^{\infty} e^{-x^2/2} \,dx = \sqrt{\pi/2}. ...is this correct? what i did i just use e^{-x^2} and substitute -x^2/2 with -x^2 ...
 
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No, you should have
\int_{-\infty}^{\infty} e^{-x^2/2} \,dx = \sqrt{2\pi}.

Unfortunately I don't know of any way to prove the Gaussian integral without using double integration.
 
d_b said:
Thank you for clearing up the problem, I haven't learn how to do double intergral yet so is there any other way of doing it without using double intergral??

also \int_{-\infty}^{\infty} e^{-x^2/2} \,dx = \sqrt{\pi/2}. ...is this correct? what i did i just use e^{-x^2} and substitute -x^2/2 with -x^2 ...
If you look at adriank's method (which is the standard for this integral), you will see that it is simply a product of two integrals, both before and after the change of variables. The only tricky part is the change from rectangular to polar coordinates.
 
  • #10
i found http://en.wikipedia.org/wiki/Gaussian_integral this online which helps...but I was just thinking if i was go havee^{x^2} can i still use the double intergral?? or is there other way of doing it? (ie. using the theory property of exponential)
 
  • #11
If you have the positive exponent ex2, then the integral will diverge.
 
  • #12
<br /> (\int_{-\infty}^{\infty}e^{-x^2}dx)^2=(\int_{-\infty}^{\infty}e^{-x^2}dx)\cdot (\int_{-\infty}^{\infty}e^{-y^2}dy)=<br /> <br /> (\int_{-\infty}^{\infty}e^{-(x^2+y^2)}dxdy)= \int_0^{2\pi}dw\int_0^\infty dr r e^{-r^2}=-\pi e^{-r^2}\vert^\infty_0=\pi<br />


THis is what i got...Also would e^x^2 be different if it is not from negative infinity to positive infinity. Could it intergral exists if i was to intergrat each term of e^x^2 ?
 
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  • #13
adriank said:
If you have the positive exponent ex2, then the integral will diverge.

it would be diverge if i was to take from negative infinity or zero to positive infinity. What if i was to take the intergral for a small section. let say from 1 to 5. Would it still be diverge??
 
  • #14
  • #15
The other way to look at this is to use the definition of the error function:
4d4a6284c0034cad3b701f8799205132.png

400px-Error_Function.svg.png

Then split your integral into 2 sections: -\infty \rightarrow0 \mbox{ and }0 \rightarrow\infty\\

\int_{-\infty}^{\infty} e^{-x^2} \,dx=\int_{0}^{\infty} e^{-x^2} \,dx-\int_{0}^{-\infty} e^{-x^2} \,dx\\

since

\int_{a}^{b} f(x) \,dx=-\int_{b}^{a} f(x) \,dx\\.

So your integral becomes

\lim_{x\to\infty}\, (erf(x)-erf(-x))\frac{\sqrt{\pi}}{2}

which is \sqrt{\pi} because \lim_{x\to\infty}\, erf(x) = 1 and \lim_{x\to-\infty}\, erf(x) = -1
 
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  • #16
is this the only way of proving \int_{0}^{a} e^{x^2} \,dx
 
  • #17
jacophile: But first you need to prove that \lim_{x\to\infty} \operatorname{erf}(x) = 1!

d_b: What about that integral are you trying to find?
 
  • #18
You already did that.
My aim was to solve

\int_{-\infty}^{\infty}e^{-x^2}\,dx

using the erf identity, not to prove it. Like I said in my post, just another way of looking at it.
 
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  • #19
Actually, can someone help me to understand why using the following substitution is wrong?
At least I am pretty sure it is...

\int_{0}^{x}e^{-z^2}\,dz

let y=z^{2}\;\rightarrow\; dy=2 z dz

\rightarrow\;z=\sqrt{y}\;\mbox{ }(\forall\,y\geq\;0)\mbox{ }\;\rightarrow\,dz= \frac{1}{2} y^{-\frac{1}{2}}\;dy

So that the integral becomes

\frac{1}{2} \;\int_{0}^{x^{2}}\;e^{-y}\;y^{-\frac{1}{2}}\,dy

If it was ok to do this one could then integrate by parts using

u=y^{-\frac{1}{2}}\;\rightarrow\;du=-\frac{1}{2} \;y^{-\frac{3}{2}}\;dy

dv=e^{-y}dy\;\rightarrow\;v=-e^{-y}

and then build a power series (with increasingly -ve powers of y), by successive integration by parts, of the form


e^{-x^{2}}\sum_{i=1}^{\infty}f(x,i)\;\;+\;\lim_{i\to\infty}I_{i}

Assuming you could show that the second term was zero...

I'm just unsure about the first substitution.
 
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  • #20
I didn't really check your work but how's that different than just rewriting

e^{x^2} = \sum_{n=0}^{\infty} \frac{x^{2n}}{n!}

And then integrating it out.
 
  • #21
Hm, its amazing what a bit of sleep will do for you.

Ok, I see the problem now: the function is not well behaved at the lower limit of the integration so that is why the substitution is not viable.
 
  • #22
adriank said:
jacophile: But first you need to prove that \lim_{x\to\infty} \operatorname{erf}(x) = 1!

d_b: What about that integral are you trying to find?

I posted a few of them. Which one are you talking about?
 

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